2019
DOI: 10.1093/mnras/stz2530
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A spectroscopic census of the Fornax cluster and beyond: preparing for next generation surveys

Abstract: The Fornax cluster is the nearest, large cluster in the southern sky, and is currently experiencing active assembly of mass. It is thus the target of a number of ongoing observing campaigns at optical, near-infrared and radio wavelengths, using state-of-the-art facilities in the Southern hemisphere. Spectroscopic redshifts are essential not only for determining cluster membership, but also kinematics within the cluster and identifying substructures. We present a compilation of all available major spectroscopic… Show more

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Cited by 32 publications
(73 citation statements)
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References 54 publications
(60 reference statements)
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“…However, Böhringer et al (2016) also show that this scatter is driven mainly by massive clusters: when their sample is split by the median X-ray luminosity of their associated cluster (corresponding to a total mass of 1.4 × 10 14 M ), the standard deviation in RM increases to 158 ± 34 rad m -2 for sources associated with clusters in the upper half of the mass range and decreases to 62 ± 11 rad m -2 for the converse sources. Our lower derived value of of 16.8 ± 2.4 rad m -2 for the RM scatter seems broadly consistent with this coarse mass dependence, given that the total mass of the Fornax cluster is only 6 +3 −1 × 10 13 M (Drinkwater et al 2001;Nasonova et al 2011;Maddox et al 2019) inside a few Mpc, which is half the mass cut value used by Böhringer et al (2016). It is also comparable to results from simulations for unrelaxed clusters of approximately the same mass (see, e.g.…”
Section: Comparison With Cluster Stacking Experimentssupporting
confidence: 81%
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“…However, Böhringer et al (2016) also show that this scatter is driven mainly by massive clusters: when their sample is split by the median X-ray luminosity of their associated cluster (corresponding to a total mass of 1.4 × 10 14 M ), the standard deviation in RM increases to 158 ± 34 rad m -2 for sources associated with clusters in the upper half of the mass range and decreases to 62 ± 11 rad m -2 for the converse sources. Our lower derived value of of 16.8 ± 2.4 rad m -2 for the RM scatter seems broadly consistent with this coarse mass dependence, given that the total mass of the Fornax cluster is only 6 +3 −1 × 10 13 M (Drinkwater et al 2001;Nasonova et al 2011;Maddox et al 2019) inside a few Mpc, which is half the mass cut value used by Böhringer et al (2016). It is also comparable to results from simulations for unrelaxed clusters of approximately the same mass (see, e.g.…”
Section: Comparison With Cluster Stacking Experimentssupporting
confidence: 81%
“…The Fornax cluster is nearby (20.64 megaparsecs; Mpc; Lavaux & Hudson 2011), but much poorer than similarly wellstudied clusters like the Virgo and Coma clusters. It has only ∼390 member galaxies (which are typically low in mass; Maddox et al 2019) and has a comparatively low total mass of 6 +3 −1 × 10 13 M (Drinkwater, Gregg & Colless 2001;Nasonova, de Freitas Pacheco, & Karachentsev 2011;Maddox et al 2019), which is one and two orders-of-magnitude less massive than the Virgo and Coma clusters, respectively. The (presently detectable) X-ray-emitting ICM is also small, extending asymmetrically outward from NGC1399 to a mere 15%-30% of the cluster's 1.96 • virial radius.…”
Section: F(φ)e 2iφλ 2 Dφmentioning
confidence: 99%
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“…We compare our spectra to spectra from the literature (shown in black; see top-left corner for details). We also show the barycentric velocity obtained from our HI spectra (vertical red line) and from optical spectra (vertical blue line; Maddox et al 2019).…”
Section: Flux Density (Jy)mentioning
confidence: 99%
“…In each panel of Fig. 3 we also show the velocity v opt derived from optical spectroscopy (Maddox et al 2019) and the barycentric HI velocity v HI derived from our ATCA spectra.…”
Section: Hi Detection Propertiesmentioning
confidence: 99%